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Titlebook: Advances in Nuclear Dynamics 5; Wolfgang Bauer,Gary D. Westfall Book 1999 Springer Science+Business Media New York 1999 CERN.Kaon.Strangen

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發(fā)表于 2025-3-28 14:35:52 | 只看該作者
42#
發(fā)表于 2025-3-28 22:02:49 | 只看該作者
Two Final Methods and Some Final Thoughtsn production is investigated. An invariance of the spectral shape and a simple scaling of the yield with the number of par-ticipating nucleons is observed for centralities with more than about 50 participants. The transverse mass spectrum is analyzed in terms of a thermal model with hydrodynamic exp
43#
發(fā)表于 2025-3-29 01:39:02 | 只看該作者
44#
發(fā)表于 2025-3-29 05:10:08 | 只看該作者
https://doi.org/10.1007/978-0-387-92710-7ach, including a non-Markovian collision term. By employing a Skyrme force, the isoscalar monopole, isovector dipole and isoscalar quadrupole excitations in .Ca are calculated. The collisional damping due to decay into incoherent 2p-2h states is small at low temperatures but increases rapidly at hig
45#
發(fā)表于 2025-3-29 09:23:34 | 只看該作者
46#
發(fā)表于 2025-3-29 14:54:40 | 只看該作者
47#
發(fā)表于 2025-3-29 18:15:26 | 只看該作者
World-Systems Evolution and Global Futures For peripheral collisions the measured charge distributions develop progressively according to a power law which can be fitted by a single r exponent independently of the bombarding energy in the range 250-1200 A MeV. In addition to this universal feature, we observe that the location of the maximu
48#
發(fā)表于 2025-3-29 23:11:38 | 只看該作者
Leonid E. Grinin,Andrey V. Korotayevnding of stars and the standard model [., .]. The precise knowledge of the astrophysical ..-factor of the .Be (p, γ) .B reaction at the Gamow peak, about 20 keV, is of crucial importance for interpreting terrestrial measurements of the solar neutrino flux [.]. This is particularly true for the inter
49#
發(fā)表于 2025-3-30 00:03:26 | 只看該作者
50#
發(fā)表于 2025-3-30 06:33:06 | 只看該作者
https://doi.org/10.1007/978-3-319-68219-8em in a potential well, thermodynamic variables such as temperature and pressure and their relationship to the excitation energy of the system are obtained. We see clearly the existence of three regions in calculated caloric curve; namely liquid-dominant, plateau and gas regions. The transition from
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